topic 9 Flashcards

(14 cards)

1
Q

electrons behave like a tiny bar magnet

A

due to intrinsic angular momentum of an electron (s)
- has magnetic moment (us)
- must be quantised

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2
Q

the orbital angular momentum of an electron with l>0 leads to

A

a second source of atomic magnetic moment ul
- magnetic moment vectors oriented in opposite direction to angular momentum vectors from which they stem from
- must be quantised (values that make up equation are quantised)

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3
Q

spin - orbit coupling

A
  • magnetic interaction between quantised spin and orbital magnetic moments of an electron
  • leads to total angular momentum J
  • internal interaction = splitting
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4
Q

Zeeman effect

A
  • external interaction between an atom and an applied magnetic field that further spilts the energy of the levels into individual states
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5
Q

in an applied magnetic field, B, energy of the magnetic moment associated with the total angular moment, uj, of an electron

A

changes
- change in energy depend on the relative orientation of the magnetic moment (quantised by Mj) and the direction of the applied field
- Zeeman effect

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6
Q

hands rules involving spin - orbit coupling

A
  • for a sub shell less than half full, lowest J = ground level
  • for a sub shell more than half full, highest J = ground level
  • for an exactly filled half - sub shell there is no spin - orbit coupling in ground state due to rules of maximum multiplicity
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7
Q

how is the hole formalism (configuration of holes and electrons give rise to the same terms) effected by spin - orbit coupling

A
  • the splitting term is reversed due to hunds 3rd rule and so pairs of electron configurations have different ground state level
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8
Q

energy of level 2s+1L (term)

A

E_L,S,J = hcA( J(J+1) - L(L+1) - S(S+1)/ all divided by 2)
- A is spin - orbit coupling constant (cm^-1)

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9
Q

coupling constant A

A
  • increases with atomic number and scales roughly as A proportion to Z^4
  • less than Half filled sub shell A>0 Such that E(J) increases as J increases
  • more than half filled sub shell A<0 such that E(J) decrease as J increases
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10
Q

lande interval rule

A
  • for levels of the same term, the values of L and S are the same
  • thus the energy spacing between levels J and J + 1
    = hcA (J + 1)
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11
Q

selection rules

A
  • change in J = 0, +/- 1
  • change in S = 0
  • change in L = 0, +/- 1 (provided change in l = +/- 1)
  • chang in n = no restrictions
  • change in Mj states = 0, +/- 1
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12
Q

spin - orbit coupling spectral line splitting

A
  • alkali metals where p electron of an electronically excited state relaxes to a lower s orbital, spin orbit coupling gives rise to important spectral feature
  • look at strong line at 589 nm under high resolution, see doublet
  • due to spin - orbit coupling
  • down the alkali metal group the splitting increases with spin - orbit coupling constant ( A proportional to Z^4)
  • doublet because line splitting from 2p3/2 to 2S1/2 and 2P1/2 to 2S1/2
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13
Q

Zeeman effect equation

A
  • E = -total angular momentum (uj) x applied magnetic field (B) = - modulus uj x modulus B x cos(theta)
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14
Q

the stronger the applied field

A

the stronger the spectral line splitting

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